JPH0697519B2 - Magneto-optical recording device - Google Patents

Magneto-optical recording device

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Publication number
JPH0697519B2
JPH0697519B2 JP32327191A JP32327191A JPH0697519B2 JP H0697519 B2 JPH0697519 B2 JP H0697519B2 JP 32327191 A JP32327191 A JP 32327191A JP 32327191 A JP32327191 A JP 32327191A JP H0697519 B2 JPH0697519 B2 JP H0697519B2
Authority
JP
Japan
Prior art keywords
magnetic
magnetic field
magnetic layer
magneto
recording
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP32327191A
Other languages
Japanese (ja)
Other versions
JPH056503A (en
Inventor
陽一 大里
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canon Inc
Original Assignee
Canon Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP32327191A priority Critical patent/JPH0697519B2/en
Publication of JPH056503A publication Critical patent/JPH056503A/en
Publication of JPH0697519B2 publication Critical patent/JPH0697519B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は磁気カー効果を利用して
読み出しすることのできるキュリー点書き込みタイプの
光磁気記録媒体を使用する重ね書き可能な光磁気記録装
置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an overwritable magneto-optical recording apparatus using a Curie point writing type magneto-optical recording medium which can be read by utilizing the magnetic Kerr effect.

【0002】[0002]

【従来の技術】消去可能な光メモリとして光磁気記録媒
体が知られている。光磁気記録媒体は、従来の磁気ヘッ
ドを使った磁気記録媒体と比べて高密度記録、非接触で
の記録再生等が可能であるという長所がある反面、記録
前に一度記録部分を消去しなければならない(一方向に
着磁しなければならない)という欠点がある。この欠点
を補うための光磁気記録装置としては、記録再生用ヘッ
ドと消去用ヘッドを別々に設けたものや、レーザーの連
続ビームを照射しつつ、同時に印加する磁界を変調しな
がら記録するものがある。が、これらの光磁気記録再生
装置は前者においては装置が大がかりなものとなってし
まい、コストも高くなってしまう。また、後者について
は高速の変調を行うことができないといった欠点があ
る。このため、本出願人は従来の装置構成に簡単な構造
の磁界発生手段を付設するだけで磁界記録媒体と同様な
重ね書き(オーバーライト)を可能とした光磁気記録方
式を以前に提案している(特願昭61−158787
号:特願昭62−20384号の優先権主張出願の基礎
出願)。すなわち、低いキュリー点(TL )と高い保磁
力(HH )を有する第1磁性層と、この磁性層に比べて
相対的に高いキュリー点(TH )と低い保磁力(HL
を有する第2磁性層からなる二層構造の垂直磁化膜を基
板上に有して成る光磁気記録媒体を使用して、該媒体に
対して、記録用ヘッドと異なる場所で、保磁力HL の第
2磁性層を一方向に磁化させるのに十分で保磁力HH
第1磁性層の磁化の向きを反転させることのない大きさ
の磁界Bを加え、次に、磁気ヘッドにより、バイアス磁
界を印加すると同時に低いキュリー点(TL )付近まで
該媒体が昇温するだけのレーザーパワーを照射すること
により、第2磁性層の磁化の向きを変えないまま第1磁
性層の磁化の向きを第2磁性層に対して安定な向きに揃
える第1種の予備記録か、バイアス磁界を印加すると同
時に高いキュリー点(TH )付近まで該媒体が昇温する
だけのレーザーパワーを照射することにより、第2磁性
層の磁化の向きを反転させて同時に第1磁性層も第2磁
性層に対して安定な向きに磁化する第2種の予備記録か
を、信号に応じて実施し、次に、該媒体を運動させて、
予備記録されたビットを前記磁界Bを通過させることに
より、第1種の予備記録により形成されたビットについ
ては第1磁性層、第2磁性層とも磁化の向きをそのまま
変化させず、第2種の予備記録により形成されたビット
については、第2磁性層の磁化の向きを前記磁界Bと同
方向に反転させ、第1磁性層については磁化の向きをそ
のまま変化させないとして二値の記録を行うものであ
る。
2. Description of the Related Art A magneto-optical recording medium is known as an erasable optical memory. The magneto-optical recording medium has an advantage that high-density recording and non-contact recording / reproducing are possible as compared with a magnetic recording medium using a conventional magnetic head, but on the other hand, the recorded portion must be erased once before recording. It has the disadvantage that it must be magnetized in one direction. As a magneto-optical recording device for compensating for this drawback, there are a magneto-optical recording device in which a recording / reproducing head and an erasing head are separately provided, and a device which irradiates a continuous laser beam and simultaneously records while modulating a magnetic field applied. is there. However, in the former case, these magneto-optical recording / reproducing devices are large-scaled and costly. Further, the latter has a drawback that high speed modulation cannot be performed. For this reason, the applicant has previously proposed a magneto-optical recording method capable of overwriting similar to a magnetic field recording medium by simply adding a magnetic field generating means having a simple structure to the conventional apparatus configuration. (Japanese Patent Application No. 61-158787)
No .: Basic application for priority claim application in Japanese Patent Application No. 62-20384). That is, the first magnetic layer having a low Curie point (T L ) and a high coercive force (H H ), and a Curie point (T H ) and a low coercive force (H L ) which are relatively higher than those of this magnetic layer.
Using a magneto-optical recording medium having a two-layered perpendicularly magnetized film having a second magnetic layer on a substrate, a coercive force H L is applied to the medium at a position different from the recording head. Magnetic field B having a coercive force H H sufficient to magnetize the second magnetic layer in one direction and does not reverse the magnetization direction of the first magnetic layer, and then a bias is applied by the magnetic head. By applying a magnetic field and at the same time irradiating laser power enough to raise the temperature of the medium to near the low Curie point (T L ), the magnetization direction of the first magnetic layer can be maintained without changing the magnetization direction of the second magnetic layer. the first type of pre-recorded or to align the stable orientation for the second magnetic layer, it at the same time high Curie point by applying a bias magnetic field (T H) near to the medium is irradiated with a laser power of only heating Reverses the magnetization direction of the second magnetic layer. The second kind of pre-recording, in which the first magnetic layer is magnetized in a stable direction with respect to the second magnetic layer at the same time, is performed according to a signal, and then the medium is moved,
By passing the magnetic field B through the prerecorded bits, the magnetization direction of the first magnetic layer and the second magnetic layer of the bit formed by the prerecording of the first type does not change and the second type does not change. For the bit formed by the preliminary recording, the direction of magnetization of the second magnetic layer is reversed in the same direction as the magnetic field B, and the direction of magnetization of the first magnetic layer is left unchanged and binary recording is performed. It is a thing.

【0003】[0003]

【発明が解決しようとする課題】前述の方法により重ね
書きを可能にしたものであるが、記録ビットの安定性を
向上させるために光磁気ディスクの第1磁性層と第2磁
性層の間に容易磁化方向が面内方向である第3磁性層を
設けて同様なプロセスを実施する場合には、磁界発生部
から発生される磁界上を光磁気ディスクが通過する際に
記録ノイズが生じる危険性がある。本発明の目的は、光
磁気ディスクの基板の垂直方向の成分と面内方向の成分
とに分離される磁界発生部からの磁界の、当該面内成分
をできるだけ除去して、記録ノイズの少ない、重ね書き
可能な光磁気記録装置を提供することにある。
Although the overwriting is enabled by the above-mentioned method, in order to improve the stability of the recording bit, it is provided between the first magnetic layer and the second magnetic layer of the magneto-optical disk. When a similar process is carried out by providing a third magnetic layer whose easy magnetization direction is the in-plane direction, there is a risk that recording noise will occur when the magneto-optical disk passes over the magnetic field generated from the magnetic field generation section. There is. An object of the present invention is to remove as much as possible the in-plane component of the magnetic field from the magnetic field generation unit that is separated into the component in the vertical direction of the substrate of the magneto-optical disk and the component in the in-plane direction to reduce recording noise. An object is to provide an overwritable magneto-optical recording device.

【0004】[0004]

【課題を解決するための手段】本発明は、磁界発生部と
光磁気記録媒体との間に磁気遮蔽板で作られ、磁界発生
部が光磁気ディスクに磁界を加える個所に当該する部分
に開口部が設けられたマスクを磁界発生部を覆うように
配置することにより、磁界発生部からの磁界の面内方向
の成分が光磁気記録媒体に加わることを防げるようにし
たものである。
According to the present invention, a magnetic shield plate is provided between a magnetic field generating section and a magneto-optical recording medium, and the magnetic field generating section has an opening at a portion where a magnetic field is applied to the magneto-optical disk. By disposing the mask provided with the portion so as to cover the magnetic field generation portion, it is possible to prevent the in-plane component of the magnetic field from the magnetic field generation portion from being applied to the magneto-optical recording medium.

【0005】なお、本発明の記録装置は、再生手段が付
設されているものも当然含む。
The recording apparatus of the present invention naturally includes a recording apparatus provided with a reproducing means.

【0006】上記本発明の記録再生装置による重ね書き
(オーバーライト)記録は、低いキュリー温度(TL
と高い保磁力(HH )を有する第1磁性層と、この磁性
層に比べて相対的に高いキュリー温度(TH )と低い保
磁力(HL )を有する第2の磁性層の両垂直磁化膜と、
第1磁性層と第2磁性層の間に設けたキュリー温度がT
L とTH の間にあり、容易磁化方向が面内方向にある第
3磁性層の希土類−遷移金属合金膜とからなる光磁気記
録媒体を用いて前記特願昭62−20384号開示のプ
ロセスと同様のプロセスにより行われる。なお記録時の
バイアス磁界に関しては、次のように設定する。
Overwrite recording by the recording / reproducing apparatus of the present invention is performed at a low Curie temperature ( TL ).
And a first magnetic layer having a high coercive force (H H ) and a second magnetic layer having a relatively high Curie temperature ( TH ) and a low coercive force ( HL ) as compared with the magnetic layer. A magnetic film,
The Curie temperature provided between the first magnetic layer and the second magnetic layer is T
It is between L and T H, easy magnetization direction of the third magnetic layer in the plane direction rare earth - transition metal alloy film and the Japanese Patent Application Sho 62-20384 DISCLOSURE process using a magneto-optical recording medium comprising The process is similar to. The bias magnetic field during recording is set as follows.

【0007】第1種の予備記録では、第2磁性層の磁化
の向きに対して安定な向きに第1磁性層の磁化が配列し
ようとする力(交換力)が働くので、本来はバイアス磁
界は必要ではない。一方、第2種の予備記録では、バイ
アス磁界は第2磁性層の磁化反転を補助する向きに設定
する。そして重ね書き可能な記録については、第1種、
第2種どちらのレーザーパワーの予備記録でも、このバ
イアス磁界の大きさ、方向を同じ状態に設定しておくこ
とが好ましい(そうでないと記録の周波数で、バイアス
磁界を変調させなければならない)。
In the first type of preliminary recording, since the force (exchange force) that the magnetization of the first magnetic layer tries to align in a direction stable with respect to the direction of the magnetization of the second magnetic layer, the bias magnetic field is originally intended. Is not necessary. On the other hand, in the second type of preliminary recording, the bias magnetic field is set in a direction to assist the magnetization reversal of the second magnetic layer. And for records that can be overwritten, the first type,
It is preferable that the magnitude and direction of the bias magnetic field are set to be the same in the preliminary recording with both laser powers of the second type (otherwise, the bias magnetic field must be modulated at the recording frequency).

【0008】上記プロセスに用いられる光磁気記録媒体
において、第1磁性層と第2磁性層の間に設けられた容
易磁化方向が面内にある第3磁性層は、第1磁性層と第
2磁性層のそれぞれの磁化が最も安定な向きに配向する
のを制限する働きをする。これは当該配向力はそれぞれ
の磁気膜中の同一の原子のスピンがそれぞれ平行になろ
うとするために発生するので、スピンが面内方向に向き
やすい第3磁性層を介しては、その配向力が働きにくく
なるためである。この第3磁性層を設けることにより記
録されたビットの安定性が向上する。すなわち第3磁性
層は磁化が面内方向を向きやすく、記録を行わないとき
には、第1,第2磁性層の磁気的な結合を弱める働きを
して記録ビットを安定にする。なお、第3磁性層の組成
を希土類元素の割合が補償組成より大きい領域に設定す
ると、記録中の温度上昇に伴い磁化が減少して基板面垂
直方向の異方性が大きくなり、第1,第2磁性層の磁気
的結合(交換結合)を強く働かせることが可能である。
これによって、第1種および第2種の記録を安定に行う
ことが可能となる。各磁性層の特性は次の通りである。
すなわち、通常は、第1磁性層のTL は70〜180
℃、HH は3〜15KOe、第2磁性層のTH は100
〜400℃、HL は0.3〜2KOe、第3磁性層のキ
ュリー点は80〜250℃、基板垂直方向に磁化が飽和
するときの印加磁界はHL よりも大きい程度の範囲にす
るとよい。各磁性層の材料には、垂直磁気異方性を示
し、かつ磁気光学効果を呈するものが利用できるが、G
dCo,GdFe,TbFe,DyFe,GdTbF
e,TbDyFe,GdTbFeCo,TbFeCo,
GdTbCo等の希土類元素と遷移金属元素との非晶質
合金が好ましい。
In the magneto-optical recording medium used in the above process, the third magnetic layer provided between the first magnetic layer and the second magnetic layer and having the in-plane easy magnetization direction is the first magnetic layer and the second magnetic layer. It serves to limit the orientation of the respective magnetizations of the magnetic layer in the most stable orientation. This orientation force is generated because spins of the same atom in each magnetic film tend to be parallel to each other, so that the orientation force is generated through the third magnetic layer in which spins are easily oriented in the in-plane direction. Is hard to work with. By providing this third magnetic layer, the stability of recorded bits is improved. That is, the magnetization of the third magnetic layer tends to be oriented in the in-plane direction, and when recording is not performed, the magnetic coupling between the first and second magnetic layers is weakened to stabilize the recording bit. When the composition of the third magnetic layer is set to a region in which the ratio of the rare earth element is larger than the compensation composition, the magnetization decreases as the temperature rises during recording and the anisotropy in the direction perpendicular to the substrate surface increases. The magnetic coupling (exchange coupling) of the second magnetic layer can be made strong.
This makes it possible to stably perform the first type and the second type recording. The characteristics of each magnetic layer are as follows.
That is, normally, T L of the first magnetic layer is 70 to 180.
C, H H is 3 to 15 KOe, and T H of the second magnetic layer is 100.
˜400 ° C., H L is 0.3 to 2 KOe, Curie point of the third magnetic layer is 80 to 250 ° C., and the applied magnetic field when the magnetization is saturated in the direction perpendicular to the substrate is preferably in a range larger than H L. . As a material for each magnetic layer, a material exhibiting perpendicular magnetic anisotropy and exhibiting a magneto-optical effect can be used.
dCo, GdFe, TbFe, DyFe, GdTbF
e, TbDyFe, GdTbFeCo, TbFeCo,
An amorphous alloy of a rare earth element such as GdTbCo and a transition metal element is preferable.

【0009】次に、本発明の作用を明確化するため、前
記のプロセスで記録したビットの安定性および記録ノイ
ズの原因について述べる。
Next, in order to clarify the operation of the present invention, the stability of the bits recorded in the above process and the cause of recording noise will be described.

【0010】第1種の予備記録で形成されたビットは磁
界Bを何回通過しても、磁化反転を起こす磁性層はな
い。よって、第1,第2,第3磁性層はそれぞれ予備記
録により安定な状態に置かれている。ところが第2種の
予備記録で形成された第2磁性層のビットは、磁界Bを
通過すると磁界Bの向きに磁化反転する。一方、第1磁
性層の保磁力は磁界Bより大きいので磁化反転は起こら
ない。さらに第3磁性層も面内方向にのみ容易磁化され
るので磁界Bでは磁化反転は起こらないはずである。
The bit formed by the first type of preliminary recording has no magnetic layer which causes magnetization reversal no matter how many times it passes through the magnetic field B. Therefore, the first, second and third magnetic layers are placed in a stable state by the preliminary recording. However, when the bit of the second magnetic layer formed by the second type of preliminary recording passes through the magnetic field B, the magnetization is reversed in the direction of the magnetic field B. On the other hand, since the coercive force of the first magnetic layer is larger than the magnetic field B, the magnetization reversal does not occur. Furthermore, since the third magnetic layer is also easily magnetized only in the in-plane direction, the magnetic field B should not cause magnetization reversal.

【0011】ところが第3磁性層の磁化は、基板面内方
向磁界の印加では、数百Oeの磁界でも反転が起こる。
そこで繰り返し磁界Bを通過すると磁界Bの基板面内方
向の成分により第3磁性層の磁化反転が起こる。この場
合に、第1磁性層がわずかでも基板面内方向に磁化され
やすい成分を有すると、強い磁気的な結合が働いて、少
しづつ再生中に、第1磁性層の基板面内方向の磁化成分
の磁化反転を生じてしまい、これが記録ノイズの原因と
なっている。
However, when the magnetic field in the in-plane direction of the substrate is applied, the magnetization of the third magnetic layer is reversed even with a magnetic field of several hundred Oe.
Therefore, when the magnetic field B is repeatedly passed, the magnetization reversal of the third magnetic layer occurs due to the component of the magnetic field B in the in-plane direction of the substrate. In this case, if the first magnetic layer has a component that is easily magnetized in the in-plane direction of the substrate, strong magnetic coupling works, and the magnetization of the first magnetic layer in the in-plane direction of the first magnetic layer is gradually increased during reproduction. The magnetization reversal of the component occurs, which causes the recording noise.

【0012】そこで磁界Bのうちの基板面内方向に磁界
成分を極力少なくする工夫が必要となる。
Therefore, it is necessary to devise to minimize the magnetic field component of the magnetic field B in the in-plane direction of the substrate.

【0013】このためには光磁気記録媒体へ、磁界発生
部よりまわり込んで到達する磁束を除くことが効果的で
ある。この点に鑑み、本発明では、磁界発生部と記録媒
体との間に開口部を有する磁気遮蔽板によるマスクを設
けて、斜方向より記録媒体へ入射する磁束を除き、開口
部より磁界発生部の発生磁界を記録媒体に加える。
To this end, it is effective to remove the magnetic flux that reaches the magneto-optical recording medium from the magnetic field generating portion. In view of this point, in the present invention, a mask of a magnetic shielding plate having an opening is provided between the magnetic field generation unit and the recording medium to remove the magnetic flux incident on the recording medium in an oblique direction, and to eliminate the magnetic field generation unit from the opening. Is applied to the recording medium.

【0014】また、磁界発生部の記録媒体を挟んだ反対
側に、同様の逆極性の磁界発生部を設ければ、さらに回
り込みにより到達する磁束を除く効果が上がる。
Further, if a similar magnetic field generator of opposite polarity is provided on the opposite side of the magnetic field generator with respect to the recording medium, the effect of removing the magnetic flux arriving due to wraparound is further enhanced.

【0015】[0015]

【実施例】光磁気ディスクを、次のように作製した。ま
ずプリグループ、プリフォーマット信号の刻まれたポリ
カーボネート製のディスク基板上にSi(シリコン)を
保護層として500Åの厚さに設けた。次に第1磁性層
Tb12GFe78(原子比)を300Åの厚さに設けた。
この第1磁性層はTL =約150℃、HH =約8KOe
で副格子磁化はFe原子の方が大であった。
Example A magneto-optical disk was manufactured as follows. First, Si (silicon) was provided as a protective layer in a thickness of 500Å on a polycarbonate disk substrate on which pre-group and pre-format signals were engraved. Next, a first magnetic layer Tb 12 GFe 78 (atomic ratio) was provided to a thickness of 300Å.
This first magnetic layer has T L = about 150 ° C. and H H = about 8 KOe.
Thus, the sublattice magnetization of the Fe atom was larger.

【0016】次に第3磁性層Tb35Fe60Co5 (原子
比)を150Åの厚さに設けた。キュリー温度は約17
0℃、面内方向が磁化容易軸で面内方向では400Gで
磁化反転が起こった。垂直方向へ磁化の向きを配向させ
るためには約3.0KOeの外部磁界が必要であった。
Next, a third magnetic layer Tb 35 Fe 60 Co 5 (atomic ratio) was provided to a thickness of 150Å. Curie temperature is about 17
The magnetization reversal occurred at 0 ° C. and the in-plane direction was the easy axis of magnetization, and 400 G in the in-plane direction. An external magnetic field of about 3.0 KOe was required to orient the magnetization in the perpendicular direction.

【0017】次に第2磁性層Tb24Fe68Co8 (原子
比)を300Åの厚さに設けた。T H =約180℃、H
L =約1.0KOeで、第2磁性層の副格子磁化はTb
原子の方が大であった。
Next, the second magnetic layer Tbtwenty fourFe68Co8 (atom
Ratio) to a thickness of 300Å. T H = Approx. 180 ° C, H
L = About 1.0 KOe, the sub-lattice magnetization of the second magnetic layer is Tb
The atom was bigger.

【0018】次にSi(シリコン)を保護層として10
00Åの厚さに設けた。
Next, Si (silicon) is used as a protective layer 10
It was set to a thickness of 00Å.

【0019】最後に上記の基板を、ホットメルト接着剤
を用いてポリカーボネート貼り合わせ用基板と貼り合せ
光磁気ディスクを作成した。
Finally, the above substrate was bonded to a polycarbonate bonding substrate using a hot melt adhesive to prepare a magneto-optical disk.

【0020】このように作成された光磁気ディスク11
を用いて図1に例示する本発明の光磁気ディスク記録再
生装置により、記録再生の実験を行った。
The magneto-optical disk 11 produced in this way
A recording / reproducing experiment was conducted by using the magneto-optical disk recording / reproducing apparatus of the present invention illustrated in FIG.

【0021】スピンドルモーター3の回転軸に上記光磁
気ディスク11をセットした。本装置において、光源4
からの出射光は、光変調装置5と偏光子13を通過して
ハーフミラー6で反射され、コイル10により上下方向
の位置を制御される対物レンズ7を通して、光磁気ディ
スク11上へ集光する。また、反射した光は、対物レン
ズ7、ハーフミラー6、検光子8を通過して光変換素子
9へと導かれ、再生信号を発生する。また、本発明は、
記録時のバイアス磁界発生用の磁石12および磁界発生
用磁石1と磁気遮蔽によるマスク2とを有する。なお、
マスク2は磁界発生部1が発生する磁束の周囲を遮蔽す
るために磁界発生部1を覆うように設けられ、磁界発生
部1により光磁気ディスク11に磁界Bを加える個所に
当該する部分に開口部が設けられている。
The magneto-optical disk 11 was set on the rotary shaft of the spindle motor 3. In this device, the light source 4
Light emitted from the laser beam passes through the optical modulator 5 and the polarizer 13, is reflected by the half mirror 6, and is focused on the magneto-optical disk 11 through the objective lens 7 whose vertical position is controlled by the coil 10. . Further, the reflected light passes through the objective lens 7, the half mirror 6, and the analyzer 8 and is guided to the light conversion element 9 to generate a reproduction signal. Further, the present invention is
It has a magnet 12 for generating a bias magnetic field during recording, a magnet 1 for generating a magnetic field, and a mask 2 for magnetically shielding. In addition,
The mask 2 is provided so as to cover the magnetic field generating portion 1 in order to shield the surroundings of the magnetic flux generated by the magnetic field generating portion 1. The mask 2 has an opening at a portion where the magnetic field generating portion 1 applies the magnetic field B to the magneto-optical disk 11. Section is provided.

【0022】磁界発生部1より基板面への磁界2KOe
である領域(ただし基板面内へは200Oe以下)を線
速度7m/secで通過させつつ、約1μm直径に集光
した830nmの波長のレーザービームを50%のデュ
ーティ比で1MHzと2MHzの周波数で変調させなが
らバイアス磁界150Oeのもとで4mwと8mwの二
値のレーザーパワーで記録を行った。その後、1.0m
wのレーザービームを照射して信号の再生を行ったとこ
ろ、二値の信号の再生ができた。繰り返し再生を続けて
も信号の劣化、ノイズの増加は見られなかった。この実
験においては磁界発生部1に使用した磁石は、フェライ
ト燒結体でできた10mm角のものであり、10mmの
正方形部分が光磁気ディスク11に向く。磁石とディス
ク基板間の距離は10mmであった。また、磁気遮蔽板
の開口は、3mmの正方形状であり、光磁気ディスク1
1との距離を3mmとして開口部が磁石の中心部上にく
るようにセットした。
Magnetic field 2 KOe from the magnetic field generator 1 to the substrate surface
While passing a region (less than 200 Oe into the substrate surface) at a linear velocity of 7 m / sec, a laser beam with a wavelength of 830 nm focused on a diameter of about 1 μm at a duty ratio of 50% at frequencies of 1 MHz and 2 MHz. Recording was performed with a binary laser power of 4 mw and 8 mw under a bias magnetic field of 150 Oe while modulating. After that, 1.0m
When a signal was reproduced by irradiating a laser beam of w, a binary signal could be reproduced. No signal deterioration or noise increase was observed even after repeated reproduction. In this experiment, the magnet used for the magnetic field generating unit 1 is a 10 mm square made of sintered ferrite, and a 10 mm square portion faces the magneto-optical disk 11. The distance between the magnet and the disk substrate was 10 mm. Further, the opening of the magnetic shielding plate has a square shape of 3 mm, and
The distance from 1 was set to 3 mm, and the opening was set on the center of the magnet.

【0023】次に、マスクに設けられる開口部の大きさ
およびマスクと光磁気ディスクとの距離を変化させ、前
述した磁界を加えたときに光磁気ディスクの基板面に加
わる垂直方向磁界と面内方向磁界を測定する実験を行っ
た結果を次表1に示す。なお、比較例1としてマスクを
取り付けない場合の実験結果を記すと垂直方向磁界と面
内方向磁界はそれぞれ2800(Oe),380(O
e)であり、再生時にはノイズが見られた。
Next, by changing the size of the opening provided in the mask and the distance between the mask and the magneto-optical disk, the vertical magnetic field applied to the substrate surface of the magneto-optical disk and the in-plane when the above-mentioned magnetic field is applied. The results of the experiment for measuring the directional magnetic field are shown in Table 1 below. As a comparative example 1, the experimental results in the case where the mask is not attached are described. The vertical magnetic field and the in-plane magnetic field are 2800 (Oe) and 380 (O
e), and noise was seen during reproduction.

【0024】[0024]

【表1】 このように比較例1でマスクを設けなかった場合には、
磁界発生部1からのディスク基板面内磁界成分が増大
し、再生時にノイズの増加が起こったが、マスクを設け
た実施例1−1〜1−5では、いずれも再生時にノイズ
の増加が起こらなかった。
[Table 1] In this way, when the mask is not provided in Comparative Example 1,
The in-plane magnetic field component of the disk substrate from the magnetic field generation unit 1 increased, and noise increased during reproduction. However, in Examples 1-1 to 1-5 in which the mask is provided, noise increases during reproduction. There wasn't.

【0025】[0025]

【発明の効果】以上説明したように本発明は、磁界発生
部からの磁界の面内方向成分が光磁気記録媒体に印加さ
れるのを妨げるマスクを設けたことにより記録ノイズが
生じる危険性を減少させることが可能になった。
As described above, according to the present invention, a mask is provided to prevent the in-plane direction component of the magnetic field from the magnetic field generator from being applied to the magneto-optical recording medium. It has become possible to reduce.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の光磁気記録装置の一実施例を示す構成
図である。
FIG. 1 is a configuration diagram showing an embodiment of a magneto-optical recording apparatus of the present invention.

【符号の説明】 1 磁界再生用磁石 2 マスク 3 モータ 4 光源 5 光変調装置 6 ハーフミラー 7 レンズ 8 検光子 9 光変換素子 10 コイル 11 光磁気ディスク 12 バイアス磁界発生部 13 偏光子[Explanation of Codes] 1 magnetic field reproducing magnet 2 mask 3 motor 4 light source 5 light modulator 6 half mirror 7 lens 8 analyzer 9 light conversion element 10 coil 11 magneto-optical disk 12 bias magnetic field generator 13 polarizer

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 垂直磁化膜から成る第1磁性層と、該第
1の磁性層に比べて相対的に高いキュリー温度と低い保
磁力とを有し、第1磁性層と交換結合した垂直磁化膜か
らなる第2磁性層と、第1および第2磁性層の間に設け
られ前記交換結合の強さを調整する容易磁化方向が面内
方向の第3の磁性層とから成る光磁気記録媒体に、記録
信号に応じて強度変調された光ビームを照射する手段、
前記媒体の光ビーム被照射部分近傍にバイアス磁界を印
加する第1の磁界発生手段及び前記光ビームの照射に先
立ち第2磁性層の磁化方向を所定方向に配向させる第2
の磁界発生手段から成る光磁気記録装置において、前記
第2の磁界発生手段と媒体との間に配され、第2の磁界
発生手段からの磁束の一部を透過する開口部を有し、第
2の磁界発生手段から発生した磁界の面内方向成分が媒
体に印加されるのを妨げる、磁気遮蔽材から形成された
マスクを有することを特徴とする光磁気記録装置。
1. A first magnetic layer made of a perpendicular magnetic film, a Curie temperature relatively higher than that of the first magnetic layer, and a coercive force lower than those of the first magnetic layer, and the perpendicular magnetization exchange-coupled with the first magnetic layer. A magneto-optical recording medium composed of a second magnetic layer formed of a film and a third magnetic layer provided between the first and second magnetic layers and having an easy magnetization direction in the in-plane direction for adjusting the strength of the exchange coupling. A means for irradiating a light beam whose intensity is modulated according to the recording signal,
A first magnetic field generating means for applying a bias magnetic field in the vicinity of the light beam irradiated portion of the medium; and a second magnetic layer for orienting the magnetization direction of the second magnetic layer in a predetermined direction prior to the irradiation of the light beam.
In the magneto-optical recording device including the magnetic field generating means, there is an opening that is arranged between the second magnetic field generating means and the medium and that transmits a part of the magnetic flux from the second magnetic field generating means. 2. A magneto-optical recording apparatus having a mask formed of a magnetic shielding material that prevents the in-plane direction component of the magnetic field generated by the magnetic field generating means from being applied to the medium.
JP32327191A 1991-12-06 1991-12-06 Magneto-optical recording device Expired - Lifetime JPH0697519B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32327191A JPH0697519B2 (en) 1991-12-06 1991-12-06 Magneto-optical recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32327191A JPH0697519B2 (en) 1991-12-06 1991-12-06 Magneto-optical recording device

Publications (2)

Publication Number Publication Date
JPH056503A JPH056503A (en) 1993-01-14
JPH0697519B2 true JPH0697519B2 (en) 1994-11-30

Family

ID=18152930

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32327191A Expired - Lifetime JPH0697519B2 (en) 1991-12-06 1991-12-06 Magneto-optical recording device

Country Status (1)

Country Link
JP (1) JPH0697519B2 (en)

Also Published As

Publication number Publication date
JPH056503A (en) 1993-01-14

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